Headset with Magnetic Frictional Coupler

ABSTRACT

A headset is described that utilizes magnetic frictional couplers. A coupler includes a first member having a first engagement surface and a second member having a second engagement surface disposed for relative positioning of the first and second members along a line of adjustment. One or more magnetic elements are arranged on the first and second members to establish a magnetic flux between the first engagement surface and the second engagement surface, and thereby establishing a frictional force tending to hold the relative positions of the first and second members. The magnetic flux varies as a function of relative position of the first and second members along the line of adjustment, and has peaks at a plurality of detent positions along the line of adjustment.

BACKGROUND OF THE INVENTION Field of the Invention

The present invention relates to frictional couplers for headsets with arotating boom for positioning a microphone or other component, and/or anadjustable headband allowing for adjusting the fit of the headset.

Description of Related Art

Headsets are used in a variety of environments. For example, headsetsare used in call centers so that the telephone operators can conductconversations with their hands free. Many types of headsets include arotating boom for positioning a microphone or other component to be usedby the person wearing the headset. Also, many types of headsets haveadjustable headbands which permit the user to adjust the length of theheadband to improve the fit.

For positioning booms and adjusting headbands, some types of headsetsrely on frictional couplers. Some frictional couplers have positionsthat are controlled by plastic-on-plastic friction with or withoutdetents. In some examples, detents can be implemented using metal orplastic springs in contact with a wave-like surface.

When headset frictional couplers are designed using metal, plasticsand/or elastomers, the frictional force tends to change as the materialswear out and creep, over the life of the product. Also, these types ofmaterials present manufacturing and production difficulties, so they aremade with tolerance that leads to variation in adjustment performanceeven when new.

It is desirable to provide headsets having more reliable adjustmenttechnologies.

SUMMARY

A headset including a magnetic frictional coupler is described thatincludes magnetic elements arranged to establish a magnetic flux thatvaries according to relative positions of elements of the frictionalcoupler. Because the magnetic elements can comprise magnets that do notchange in magnetic force over time, problems arising as prior artfrictional couplers wear out can be reduced or eliminated. Also, themagnetic frictional couplers for headsets described herein can be small,can operate silently and can be easily manufactured.

An embodiment is described in which the headset comprises a first memberhaving a first engagement surface and a second member having a secondengagement surface disposed for relative positioning of the first andsecond members along the line of adjustment. Magnetic elements arearranged on the first and second members. The magnetic elements arearranged to establish a magnetic flux between the first engagementsurface and the second engagement surface, and thereby establishing africtional force tending to hold the relative positions of the first andsecond members, at least in selected detent positions. The magnetic fluxvaries as a function of the relative positions of the first and secondmembers along the line of adjustment, and has peaks at a plurality ofdetent positions along the line of adjustment. In some embodiments, thefirst and second members comprise a hub and a boom configured forrotational positioning around a pivot to adjust the angle of the boom.In some embodiments, the first and second members comprise elements ofthe headband configured for translational positioning to adjust thelength of the headband.

The magnetic elements can comprise various combinations of permanentmagnets, elements made of ferromagnetic materials which can bemagnetized by an imposed magnetic field, thin-film magnets comprisingpatterned or “printed” magnetic fields, and/or other magnetic materialssuitable for inducing magnetic flux. In some embodiments, one or more ofthe magnetic elements can be an electromagnet.

In one example, a plurality of magnets is fixed on the first member,arranged with one magnetic pole proximal to the first engagement surfaceand an opposite magnetic pole distal to the first engagement surface. Inthis configuration, the poles of the magnets proximal to the firstengagement surface are disposed in a pattern corresponding to the detentpositions. Also, a complementary magnetic element, or set of elements,is disposed on the second member, arranged to increase the magnetic fluxwhen the second member is positioned at detent positions in theplurality of detent positions.

In some embodiments, the one or more magnetic elements can comprise anelongated magnetic strip disposed along the line of adjustment on thefirst member, and a complementary magnetic element on the second member.The elongated magnetic strip and complementary magnetic element cancooperate to establish a minimum attractive magnetic flux, andcorresponding frictional force, along the line of adjustment.

Also, in some embodiments, a non-magnetic spacer can be disposed betweenthe first and second members. The spacer can comprise a material havinga selected coefficient of friction (e.g. a lower coefficient offriction) which contributes a selected amount to the frictional force.Also, the spacer can have a specified thickness which can modify themagnitude of the magnetic flux at the engagement surfaces. The spacercan be part of one of the first and second members, or a separateelement as suits a particular implementation.

Other aspects and advantages of the present technology can be seen onreview of the drawings, the detailed description and the claims whichfollow.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a simplified diagram of a telephone headset having magneticfrictional couplers as described herein for the microphone boom and forthe adjustable headband.

FIGS. 2A, 2B, 2C illustrate rotational adjustment of a microphone boomfor the headset of FIG. 1.

FIG. 3 illustrates a magnetic frictional coupler for a microphone boomaccording to an embodiment described herein.

FIG. 4 is a simplified graph of magnetic flux versus relative angle fora magnetic frictional coupler like that of FIG. 3.

FIG. 5 illustrates a non-magnetic spacer between first and secondmembers of a magnetic frictional coupler.

FIG. 6 is an exploded view of components of a magnetic frictionalcoupler like that of FIG. 3 taken from a first perspective.

FIG. 7 is an exploded view of components of the magnetic frictionalcoupler of FIG. 6 taken from a different perspective.

FIGS. 8A, 8B illustrate a plurality of magnetic elements on a firstmember and complementary magnetic elements on a second member arrangedto establish a magnetic flux that is a function of relative rotationalposition.

FIG. 9 is an alternative arrangement of magnetic elements on the secondmember which can be used as a complement to the configuration of FIG.8A.

FIG. 10 is an alternative arrangement of magnetic elements, in the formof a patterned magnetic film, on one of the first and second members.

FIG. 11 illustrates a magnetic frictional coupler for an adjustableheadband according to an embodiment described herein.

FIG. 12 is a simplified graph of magnetic flux versus relativetranslational distance for a magnetic frictional coupler like that ofFIG. 11.

FIG. 13 is an exploded view of components of a magnetic frictionalcoupler like that of FIG. 11 taken from a first perspective.

FIG. 14 is an exploded view of components of the magnetic frictionalcoupler of FIG. 13 taken from a different perspective.

FIG. 15 illustrates an arrangement of magnetic elements for first andsecond members of a magnetic frictional coupler arranged fortranslational positioning.

FIG. 16 illustrates an arrangement of magnetic elements on the secondmember for the embodiment of FIG. 15.

FIG. 17 illustrates an alternative arrangement of magnetic elements forfirst and second members of a magnetic frictional coupler arranged fortranslational positioning.

FIG. 18 illustrates an arrangement of magnetic elements for the secondmember for the embodiment of FIG. 17.

FIG. 19 illustrates an alternative implementation of a boom hub and boomwith a magnetic frictional coupler.

FIG. 20 is an aerial view of the boom hub and boom of FIG. 19.

FIG. 21 is a simplified graph of magnetic flux versus relative angle fora magnetic frictional coupler like that of FIG. 20.

DETAILED DESCRIPTION

A detailed description of embodiments of the technology described hereinis provided with reference to the FIGS. 1-21.

FIG. 1 is a simplified illustration of a headset 10 having a headbandcomprising a first member 11 and a second member 12 which are connectedat their proximal ends by a magnetic frictional coupler 13 fortranslational adjustment. Speaker housings 15 and 16 are disposed on thedistal ends of the members 11 and 12, respectively. The headset 10 alsohas a microphone boom 18 connected at its proximal end to a magneticfrictional coupler 19 connected to the speaker housing 15 or firstheadband member 11, for rotational adjustment. A microphone 20 isdisposed on the distal end of the microphone boom 18.

The magnetic frictional coupler 13 for headband length adjustment andthe magnetic frictional coupler 19 for the microphone boom angleadjustment include means for establishing a magnetic flux (measured forexample in Webers W) which is a function of relative position of thefirst member 11, 15 and the second member 12, 18 along a line ofadjustment. Such means can be implemented using one or more magneticelements on the first and second members, arranged in a pattern toestablish variations in flux as a function of relative position,examples of which are described with reference to FIGS. 13, 15, 17 and19. As mentioned above, the magnetic elements can comprise variouscombinations of permanent magnets, elements made of ferromagneticmaterials which can be magnetized by an imposed magnetic field,thin-film magnets comprising patterned or “printed” magnetic fields,and/or other magnetic materials suitable for inducing magnetic flux. Insome embodiments, one or more of the magnetic elements can be anelectromagnet.

Peaks in the magnetic flux establish detent positions for theadjustment, having higher static frictional force that results from thepeak magnetic flux. The pattern of magnetic elements on the first memberand the corresponding pattern of magnetic elements on the second membercooperate to establish a complex magnetic field. The magnetic flux isthe summation or integral of the field (measured for example in teslasor W/m²) over the area of engagement between the first and secondmembers, and is a measure of the normal force and correspondingfrictional force at the surfaces of engagement. As the relativepositions of the magnetic elements in the patterns on the first andsecond members change, the magnetic field changes and the magnetic fluxchanges. Thus, the magnetic force of attraction and correspondingfrictional force between the first member 11 and the second member 12 atthe magnetic frictional coupler 13 vary as the first and second membersslide along the line of adjustment.

FIGS. 2A-2C are simplified side views of a headset like that of FIG. 1,showing rotation of the microphone boom 18 relative to a boom hub in themagnetic frictional coupler 19. Reference numerals used in FIGS. 2A-2Care the same as those used in FIG. 1, for like elements. FIG. 2Aillustrates a relative angle θ of roughly 120° measured from thevertical line defined by the first member 11 of the headband. FIG. 2Billustrates a relative angle θ of roughly 90° measured from the verticalline defined by the first member 11 of the headband. FIG. 2C illustratesa relative angle θ of roughly 105° measured from the vertical linedefined by the first member 11 of the headband. In some embodiments, therange of rotation of a microphone boom can be 360°. In other examples,the range of rotation can be limited to 270° or less.

The magnetic frictional coupler 19 includes means for establishing amagnetic flux that is a function of relative rotational position of themicrophone boom 18 and the first member 11 of the headband, which can bemeasured as a relative angle between the microphone boom 18 and the boomhub at the magnetic frictional coupler 19. Such means can be implementedusing one or more magnetic elements on the boom and the hub, arranged ina pattern to establish variations in flux as a function of relativeangle θ. Examples of such means are described with reference to FIGS.6-10. Peaks in the magnetic flux establish detent angles for theadjustment. Thus, the magnetic force of attraction and correspondingfrictional force between the boom 18 and the hub at the magneticfrictional coupler 19 vary as the first and second members rotate arounda circular line of adjustment.

FIG. 3 illustrates an example of a magnetic frictional coupler for amicrophone boom. The coupler includes a first member comprising a boomhub 30 (which can be on or part of a speaker housing) and a secondmember comprising a microphone boom 32 with a bearing member 31 coupledto a pivot pin 33 on the boom hub 30. In the illustrated example, anon-magnetic spacer 34 is disposed between an engagement surface on thebearing member 31 and a corresponding engagement surface on the boomhub. As illustrated, the magnetic frictional coupler shown in FIG. 3comprises an arrangement of magnetic elements creating a magnetic fluxthat changes as a function of the relative angle θ.

FIG. 4 is a graph showing variations in magnetic flux as a function ofrelative angle between the microphone boom 32 and the boom hub 30. Inthe example illustrated by FIG. 4, the magnetic flux varies as asinusoid as the relative angle increases, so that there is a pluralityof peaks 41, 42, 43, 44 . . . in the magnetic flux as the angle changes.The peaks correspond with detents in the rotational angle of the boom.The magnetic field will tend to hold the boom in a positioncorresponding to a peak in magnetic flux. Also illustrated in FIG. 4,there is a minimum magnetic flux 48 established by the patterns ofmagnetic elements across the range of motion of the coupler. The minimummagnetic flux 48 in this example is an attracting force (positive onthis graph). In other embodiments, with suitable guide structures, theminimum magnetic flux can be a repelling force (negative) in one or moreselected positions. This minimum magnetic flux 48 can be established bythe pattern of magnetic elements to maintain a minimum force ofattraction between the members of the coupler. This is a simplifiedexample, because the magnetic flux can be a function of relative anglemore complex than a simple sinusoid, depending on the pattern ofmagnetic elements in the magnetic frictional coupler. For example, FIG.4 shows peaks and valleys in the magnetic flux of uniform magnitude. Insome embodiments, there are peaks and valleys of varying magnitudedisposed along the line of adjustment.

FIG. 5 is a simplified illustration of a magnetic frictional couplerhaving a non-magnetic spacer disposed between the members of thecoupler. In this example, the coupler includes a first member 51, suchas a boom hub like that of FIG. 3, and a second member 52, such as abearing member of a microphone boom like that of FIG. 3. A non-magneticspacer 53 is disposed between the first member 51 and the second member52. The non-magnetic spacer 53 has a thickness T which separates themagnetic elements on the first and second members, thereby limiting theintensity of the magnetic fields between particular magnetic elements onthe members. By specifying the thickness T, the intensity of themagnetic field can be designed so that the magnetic flux and frictionalforce induced fall within acceptable ranges for ease-of-use by theconsumer, while maintaining strong detents. Also, the non-magneticspacer 53 can comprise a material having a specified coefficient offriction, such as a low friction material, or other materials that arechosen for the purpose of establishing preferred ranges of frictionalforce in the magnetic frictional coupler on the engagement surfaces 54,55 of the first member 51 and the second member 52. Examples ofmaterials that can be utilized include Delrin, nylon, Teflon coatedmaterials, and so on.

In the illustrated embodiment, the spacer 53 comprises a separatecomponent disposed between the first and second members havinginterfaces at which the engagement surfaces are slidably engaged on atleast one side of the spacer. In other embodiments, the spacer 53 can beincorporated in the body of, or fused with, one of the first and secondmembers. It is preferred that the material of the spacer be differentthan the material on the engagement surface or surfaces against which itis slidably engaged.

In the example shown, the engagement surfaces are flat to support smoothsliding as the members of the magnetic frictional coupler are adjustedin position. In other embodiments, the engagement surface on one or bothof the members can have one or more features such as bumps or waves tosupport formation of detents.

FIGS. 6 and 7 illustrate an exploded view of components of a magneticfrictional coupler like that shown in FIG. 3, from opposingperspectives. The elements shown can be made of a variety of plasticsand other suitable structural materials, such as aluminum, and bycombinations of such materials, by injection molding, machining andother techniques. With reference to FIG. 6, a boom hub 100 is coupled toa boom 102 having a bearing member 101 by the magnetic frictionalcoupler. The engagement surface of the boom is on an opposite surface ofthe bearing member hidden from view in this perspective (see surface 131in FIG. 7). The boom hub 100 includes a pivot pin 104 protruding on anaxis of the hub 100. A circular recess 105 in an engagement surface 110of the hub is disposed around the pin 104, and shaped to receive acorresponding arcuate magnetic element 115, which in this embodiment isa closed ring-shaped element. Also, the pattern of holes 106, 107, . . .111 is arrayed on the surface 110 with spaces therebetween outside thecircular recess 105. The holes 106, 107, . . . 111 are shaped to receivecorresponding magnetic elements which can comprise bar magnets 116, 117,. . . 121. When the bar magnets 116, 117, . . . 121 are positioned inthe holes 106, 107, . . . 111, one pole of each bar magnet is disposedproximal the engagement surface 110, and an opposite pole of each barmagnet is disposed distal from the engagement surface 110, recessedwithin the body of the hub 100. In one example, the same pole, such asthe north pole, is disposed proximal to the engagement surface 110 forevery magnet 116, 117, . . . 121 in the pattern. In an alternative, thepoles can be arranged alternately with some south poles proximal to theengagement surface and some north poles proximal to the engagementsurface.

The exposed ends of the magnetic elements can be flush with the surface110, or recessed relative to the surface, or protrude from the surfaceas suits a particular implementation. Also, a protective layer or spacerlayer can be formed over the magnetic elements.

The combination of the arcuate magnetic element 115 and the bar magnets116, 117, . . . 121, comprise a pattern of magnetic elements on the hub100, corresponding to a first member of the magnetic frictional coupler.

Also shown in FIG. 6 is a non-magnetic spacer 122 such as described withreference to FIG. 5 having a hole in the center to receive the pivot pin104.

FIG. 6 illustrates a ring-shaped magnet 125, and a bar magnet 126 to bedisposed in an engagement surface of the bearing member 101 on themicrophone boom 102. These magnets establish a pattern of magneticelements on the bearing member 101.

FIG. 6 illustrates the bearing member 101 of the boom 102, with a holein the center designed to receive the pin 104.

FIG. 7 shows the frictional magnetic coupler in an exploded view from anopposing perspective, in which the engagement surface 131 of the bearingmember 101 on the boom 102 is shown. As illustrated, a circular recess135 is disposed on the engagement surface 131 around a hole 130 that isdesigned to receive the pivot pin 104. The circular recess 135 isconfigured to receive a corresponding ring-shaped magnet 125. Also, ahole 136 is disposed in the engagement surface 131, designed to receivea bar magnet 126. The bar magnet 126 can be disposed so that one of thepoles is proximal to the engagement surface 131, and the opposing poleis distal to, and recessed in the body of the bearing member 101,relative to the engagement surface 131. Thus, the arcuate magnet, andthe bar magnet are elements in a plurality of magnetic elements arrangedin a pattern on the bearing member 101.

The exposed ends of the magnetic elements can be flush with the surface131, or recessed relative to the surface, or protrude from the surface,as suits a particular implementation. A protective layer can be disposedover the magnetic elements.

The non-magnetic spacer 122 overlies the engagement surface 131, and thepattern of magnetic elements on the bearing member 101 of the boom 102.The pattern of magnetic elements 115-121 which are disposed in the hub100 as discussed above are also illustrated in FIG. 7.

The patterns of magnetic elements used to establish magnetic flux as afunction of rotational angle can be configured as suits a particularimplementation, and the type and locations of detents desired. FIG. 8Aand FIG. 8B illustrate an alternative pattern of magnetic elements on afirst member 200 and a second member 250. In the pattern of FIG. 8A,magnetic elements 210-217 are arranged around the circumference of firstcircular member 200 with equal spacing, with a gap (in an arc from about350 degrees to about 10 degrees for example) in the spacing between thefirst magnetic element 210 and the last magnetic element 217. Aring-shaped magnet 205 (or other arcuate magnet) is disposed inside themagnetic elements 210-217. In other embodiments, the ring-shaped magnetor other arcuate magnet can be placed outside the pattern of magneticelements 210-217. A hole 201 for accepting a pivot pin is shown. Acomplementary pattern on member 250 is shown in FIG. 8B. Thecomplementary pattern includes a ring-shaped magnet 255 which is similarto the ring-shaped magnet 205 on the first member. Ring-shaped magnet255 can be configured so that the pole proximal to the engagementsurface on member 250 is the opposite pole relative to that of themagnet 205 proximal to the engagement surface on the member 200. Also,it can be configured so that the ring-shaped magnet 255 is replaced by amagnetic element in the form of a ferromagnetic ring, which is not apermanent magnet. The complementary pattern shown in FIG. 8B alsoincludes a single magnet 260 arranged in a position on member 250 tooverlie a corresponding magnet in the array of magnetic elements 210-217on the member 200. A hole 251 for accepting a pivot pin is shown. Thus,the magnetic flux is a function of the position of the magnet 260 onmember 250 relative to the positions of the magnetic elements 210-217.As the member 250 is rotated relative to the member 200, the magneticflux will change as a function of the changes in these relativepositions.

FIG. 9 illustrates (in a reduced scale) an alternative pattern ofmagnetic elements on a member complementary to the member shown in FIG.8A. In FIG. 9, the pattern comprises a single magnetic element 280 in aposition on member 270 arranged to overlie a corresponding magnet in thearray of magnetic elements 210-217 on the member 200. A hole 271 foraccepting a pivot pin is shown. The magnetic element 280 can be largerthan the magnet 260 in the embodiment of FIG. 8B in order to interactmore strongly with the ring-shaped magnet 205 on the member shown inFIG. 8A. The embodiment of FIG. 9 omits the ring-shaped magnet 255 shownin the embodiment of FIG. 8B, and can be utilized as long as the minimummagnetic force achieved is sufficient for the purposes of theimplementation.

As mentioned above, the magnetic elements can comprise permanentmagnets, ferromagnetic materials, thin-film magnets comprising patternedor “printed” magnetic fields, or other magnetic materials suitable forinducing magnetic flux. In some embodiments, one or more of the magneticelements can be an electromagnet.

FIG. 10 illustrates an embodiment using a patterned thin-film magnetdisposed on a member 300 of a magnetic frictional coupling. In theillustrated example, the pattern comprises a ring-shaped element 302with cog-shaped elements 310, 311, . . . 315 arrayed around thering-shaped element 302. A hole 301 for accepting a pivot pin is shown.The pattern shown in FIG. 10 can be used in conjunction with a patternlike that of FIG. 8B, a pattern like that of FIG. 9, or other patternsas suits a particular implementation. Also, a complementary magnet canbe formed using a thin-film magnet configured to interact with thecog-shaped elements to establish magnetic flux. A thin-film magnet canbe patterned with both north pole regions and south pole regionsproximal to the engagement surface of the member. See for examples ofpatterned thin-film magnets, Fullerton et al., U.S. Pat. No. 8,179,219entitled FIELD EMISSION SYSTEM AND METHOD, issued May 15, 2012, which isincorporated by reference as if fully set forth herein.

FIG. 11 illustrates an example of a magnetic frictional coupler fortranslational adjustment of a headset headband. The coupler includes afirst member 83 and a second member 81 disposed for translationalmovement along the axis X. The first member 83 can be coupled to a firstmember of a headset headband, and the second member 81 can be coupled toa second member of the headset headband. As the coupler is adjusted, thelength of the headband is adjusted. The first member 83 incorporates arail or guide to confine motion of the second member 81 along the lineof adjustment. A cover 82 overlies the first member 83, and secures thesecond member 81 to the rail or guide. Fasteners 85 can be used to fixthe cover 82 to the assembly. As illustrated, the magnetic frictionalcoupler shown in FIG. 11 comprises an arrangement of magnetic elementscreating a magnetic flux that changes as a function of the relativeposition along the axis X.

FIG. 12 is a graph showing variations in magnetic flux as a function ofrelative position (distance between reference locations on the members)along the axis X. In the example illustrated by FIG. 12, the magneticflux varies as a sinusoid as the relative distance of overlap betweenthe members changes, so that there is a plurality of peaks 91-94 in themagnetic flux as the distance changes. The peaks correspond with detentsin the translational position of the coupler. The magnetic field willtend to draw the position of the members of the coupler to a position ata peak in magnetic flux. Also illustrated in FIG. 12, there is a minimummagnetic flux 98 established by the patterns of magnetic elements acrossthe range of motion of the coupler. This minimum magnetic flux 98 can beestablished by the pattern of magnetic elements as discussed herein, tomaintain a minimum force of attraction between the members of thecoupler. As with FIG. 4, this is a simplified example, because themagnetic flux can be a function of the relative distance that is morecomplex than a simple sinusoid, depending on the pattern of magneticelements in the magnetic frictional coupler. For example, peaks andvalleys of the magnetic flux can vary in magnitude along the line ofadjustment.

FIGS. 13 and 14 illustrate an exploded view of a magnetic frictionalcoupler like that shown in FIG. 11, from opposing perspectives. FIG. 13shows a first member 83 that is coupled to a second member 81 by themagnetic frictional coupler. In this example, the first and secondmembers are straight. In other embodiments, the first and second membersare bowed in a manner that facilitates fitting on a user's head. Thefirst member 83 includes a guide formed by protruding rails (e.g. 401)along the sides of the member 83 configured to receive the second member81 in a sliding relationship. A cover 82 is configured to connect to themember 83, and secure the second member 81 on the guide.

An elongated recess 408 is disposed on an engagement surface 409 of themember 83, and shaped to receive a corresponding elongated magneticelement 418. Also, a pattern of holes (e.g. 402) in the engagementsurface 409 with spaces therebetween is arrayed along the elongatedrecess 408, and shaped to receive corresponding magnetic elements 411,412, . . . 415. The magnetic elements 411, 412, . . . 415 can comprisebar magnets which can be positioned in the holes (e.g. 402) so that onepole of each bar magnet is disposed proximal to the engagement surface409 of the member 83, and an opposite pole of each bar magnet isdisposed distal from the engagement surface 409, recessed within thebody of the member 83. In one example, the same pole, such as the northpole, is disposed proximal to the engagement surface 409 for everymagnet used as a magnetic element 411, 412, 415. In an alternative, thepoles can be arranged alternately with some south poles proximal to theengagement surface 409 and some north poles proximal to the engagementsurface 409.

The exposed ends of the magnetic elements can be flush with theengagement surface 409, or recessed relative to the surface, or protrudefrom the surface as suits a particular implementation. A protectivecover can be formed over the magnets.

The combination of the elongated magnetic element 418 and the barmagnets used as the magnetic elements 411-415, comprise a pattern ofmagnetic elements on the first member 83 of the magnetic frictionalcoupler.

Also shown in FIG. 13 is a non-magnetic spacer 420, such as thatdescribed above with reference to FIG. 5.

FIG. 13 illustrates an elongated magnet 435, and a bar magnet 431, whichare arranged as magnetic elements on an engagement surface of the secondmember 81. The elongated magnet 435 can be substantially longer than theelongated magnetic element 418 on the first member 83, to allow for along range of motion for the second member 81 relative to the firstmember 83.

FIG. 14 shows the frictional magnetic coupler of FIG. 13 in an explodedview from an opposing perspective, in which the engagement surface 442of the second member 81 on the magnetic frictional coupler is shown. Thesecond member 81 includes a recess 445 in the engagement surface 442configured to receive the elongated magnet 435. Also, the second member81 includes a recess 441 in the engagement surface 442 configured toreceive the bar magnet 431. Thus, the elongated magnet 435 and the barmagnet 431 are arranged in a pattern on the second member, whichcooperates with the pattern of magnetic elements on the first member toestablish a magnetic flux that is a function of the translationalposition of the first and second members.

The patterns of magnetic elements used to establish magnetic flux as afunction of translational position in the magnetic frictional couplerdescribed herein can be configured as suits a particular implementation,and the type and locations of the detents desired. FIG. 15 and FIG. 16illustrate an alternative pattern of magnetic elements on a first member501 and a second member 502. In the pattern of FIG. 15, bar or spotmagnetic elements 520-525 are arranged in a row along one side of thefirst member 501 along a line of adjustment. An elongated magnet 510 isdisposed parallel to the row of bar or spot magnetic elements 520-525.Magnetic elements 540 and 541 are disposed on the second member 502 inlocations designed to cooperate with the row of magnetic elements520-525 on the first member 501. Likewise, an elongated magnet 530 isdisposed on the second member 502 parallel with the line of adjustment,so that it overlaps with the elongated magnet 510 on the first member501, as the members are moved along the line of adjustment. In theillustration of FIG. 15, the first and second members 501, 502 arepositioned so that magnetic elements 540 and 541 on the second member502 overlap with the magnetic elements 524 and 525 in the row ofmagnetic elements on the first member 501. Thus, the relativepositioning shown in FIG. 15 can correspond to a peak in magnetic flux,and a detent in the translational motion of the members. FIG. 16illustrates the second member 502 of FIG. 15, without the overlay of thefirst member. The same reference numbers are used, and are not describedagain.

FIGS. 17 and 18 illustrate another alternative pattern of magneticelements on a first member 601 and a second member 602, which can beused in a magnetic frictional coupler for translational motion asdescribed herein. In the pattern of FIG. 17, a row of elongated magneticelements 620-625 is disposed on the first member 601. The magneticelements 620-625 are disposed so that their long axes are orthogonal tothe line of adjustment, and so that there are spaces between themagnetic elements. On the second member 602, a first elongated element640 and a second elongated element 641 are disposed in a manner tocooperate with the magnetic elements 620-625 on the first member 601 toestablish a magnetic flux that varies as a function of relative positionof the members. The complementary pattern on the second member 602 shownin FIG. 17 includes two elongated magnets orthogonal to the line ofadjustment configured for cooperation with corresponding magnets on thefirst member 601. The elongated magnets 530, 550 which are disposedparallel with the line of adjustment in the example of FIGS. 15 and 16are omitted in this example.

As illustrated in FIG. 17, the first and second members are positionedso that the magnetic elements 640, 641 on the second member 602 overlapwith the magnetic element 624, 625 on the first member 601. Thus, a peakin the magnetic flux can be formed by this positioning of the patternsof magnetic elements, establishing a detent in the magnetic frictionalcoupling.

FIG. 18 illustrates the second member 602 of FIG. 17, without theoverlay of the first member. The same reference numbers are used, andnot described again.

FIGS. 19 and 20 illustrate another example of a magnetic frictionalcoupler for a microphone boom. The coupler includes a first membercomprising a boom hub 610 and a second member comprising a microphoneboom 601. The microphone boom 601 includes a bearing member 602. Theboom hub 610 has a protruding structure 611, having a cylindricaloutside surface 613. In this embodiment, the protruding structure 611includes an opening 612. The opening 612 can also be cylindrical asshown in this illustration.

The bearing member 602 on the microphone boom 601 includes an openinghaving a cylindrical inside surface 603. Also, the outside surface 604of the bearing member 602 can be cylindrical as shown in theillustration.

Of course, in other embodiments, the opening 612 in the protrudingstructure 611 and the outside surface 604 of the bearing member 602 (aswell as other elements of the frictional coupler) can have other shapesas suits the needs of a particular implementation and for ornamentalreasons.

In the embodiment shown in FIG. 19, the opening 612 in the protrudingstructure 611 provides space for an electronic component 615. The spacemay allow for mounting of the electronic component 615 on a surface ofthe boom hub 610, or otherwise inside or accessible through the openingin the protruding structure 611. In one embodiment, the boom hub 610 isdisposed on a speaker housing for a headset. The speaker housing isconfigured to be placed over the user's ear. The electronic component615 can comprise a pushbutton, or other electronic switch, which isdisposed ergonomically centered on the speaker housing so that whendepressed or otherwise operated, the speaker housing is not displacedfrom its position over the ear.

In the example shown in FIG. 19, the first engagement surface of thefrictional coupler is on the cylindrical outside surface 613 of theprotruding structure 611. The second engagement surface of thefrictional coupler is on the cylindrical inside surface 603 of thebearing member 602. Although not shown in the figure, there may beadditional guide elements on the boom hub 610 and the bearing member 602to hold the components together during rotational movement, such as alip on the protruding member, or the like.

A pattern of magnetic elements is disposed on the cylindrical insidesurface 603 of the bearing member 602, including magnetic elements 650and 651. Likewise, a pattern of magnetic elements is disposed on thecylindrical outside surface 613 of the protruding structure 611including magnetic elements 652-656 in the drawing. Thus, the frictionalcoupler illustrated in FIGS. 19 and 20 comprises an arrangement ofmagnetic elements creating a magnetic flux that changes as a function ofthe relative angle between the microphone boom 601 and the boom hub 610.The illustrated arrangement of magnetic elements is one example. Inother examples, the continuous magnetic strip can be disposed around oneor both of the engagement surfaces. Also, printed magnetic fields can beimplemented on one or both of the engagement surfaces to create avariety of effects on magnetic flux as a function of the relative angle.As mentioned above, the magnetic elements can comprise permanentmagnets, ferromagnetic materials, thin-film magnets comprising patternedor “printed” magnetic fields, or other magnetic materials suitable forinducing magnetic flux. In some embodiments, one or more of the magneticelements can be an electromagnet.

FIG. 20 is an aerial view of a magnetic frictional coupler like that ofFIG. 19, including a boom 601 having a bearing member 602, and a hub 610having a protruding structure 611. The cylindrical outside surface ofthe protruding structure 611 and the cylindrical inside surface of thebearing member 602 are concentrically mounted in a manner that allowsfor rotation around the axis of the concentric cylindrical surfaces (603and 613 shown in FIG. 19). The arrangement of magnetic elements createsa magnetic flux that includes a component (vector) orthogonal to theaxis of rotation of the boom 601. The magnetic flux can have componentsthat are radially arranged, as illustrated by the field vector arrows(e.g. 665). As discussed above, the magnetic elements on the protrudingstructure 611 can be configured so that they have a north pole proximalto the first engagement surface, while the magnetic elements on thebearing member 602 can be configured so that they have a south poleproximate to the second engagement surface, creating regions of strongmagnetic attraction when the magnetic elements of opposite poles arealigned. Alternatively, some magnetic elements on the first and secondengagement surfaces can be configured to have an opposite pole proximalto the surfaces. Also, there can be a variety of arrangements includingboth north and south pole regions on one or both of the first and secondengagement surfaces.

The magnetic frictional coupler magnetically couples the boom 601 andthe hub 610, by a magnetic field in the region 660 between theengagement surfaces of the bearing member 602 and the protrudingstructure 611, with a corresponding normal force and friction. In someembodiments, a non-magnetic spacer can be disposed in the region 660. Insome embodiments, roller bearings or other mechanical structures forcontrolling friction between the engagement surfaces can be included.

In some embodiments, the magnetic flux can comprise a repelling force atsome relative angles of rotation, and an attracting force at otherrelative angles of rotation. The arrangement of magnetic elements can beconfigured to induce repelling force in a radially symmetric pattern insome embodiments, at some relative angles. This arrangement can be anarc, or a set of arcs, in which there is low friction in the couplingbetween the members, disposed among detents of relatively high frictionin the coupling between the members.

FIG. 21 is a graph showing variations in magnetic flux as a function ofrelative angle between the microphone boom 601 and the boom hub 610. Inthe example illustrated by FIG. 21, the magnetic flux varies as asinusoid as a relative angle increases, so that there is a plurality ofpeaks 71, 72, 73, 74 . . . in attractive magnetic flux (positive in thefigure) as the angle changes. These peaks correspond with detents in therotational angle of the boom. The magnetic field as illustrated in FIG.21 includes regions of repelling magnetic flux magnitude at minima atthe level 78 in the sinusoid (negative in the figure). As discussedabove the magnetic flux can be a function of relative angle that is morecomplex than the simple sinusoid illustrated.

A magnetic frictional coupler technology has been described for use inheadsets for the adjustment of the angle of rotation of a microphoneboom or similar boom, and for changing the length of the headband foradjustment of the fit of the headset. The use of patterns of magneticelements allows for the creation of a baseline magnetic and frictionalforce as well as detents established by peaks in magnetic and frictionalforce along the line of adjustment.

A magnetic frictional coupler as described herein can include a fixedmember and a sliding member (which can slide in a longitudinal orrotating manner) having patterns of magnetic elements or printedmagnetic fields disposed thereon.

Magnetic elements can be utilized for which the magnetism does not varyover time. Thus, the magnetic flux and frictional force induced by thepatterns of the magnetic element will not wear out, allowing for theheadband friction and detents to be maintained and remain constant overthe life of the product. Also, the magnetic frictional couplers can bemanufactured using a smaller number of parts, and without mechanicalsprings.

While the present invention is disclosed by reference to the preferredembodiments and examples detailed above, it is to be understood thatthese examples are intended in an illustrative rather than in a limitingsense. It is contemplated that modifications and combinations willreadily occur to those skilled in the art, which modifications andcombinations will be within the spirit of the invention and the scope ofthe following claims. What is claimed is:

1. A headset comprising: a first member having a first engagementsurface; a second member having a second engagement surface, the secondengagement surface disposed for movement relative to the firstengagement surface along a line of adjustment; and magnetic elementsfixed on the first and second members; the magnetic elements arranged toestablish a magnetic flux between the first engagement surface and thesecond engagement surface, the magnetic flux varying as a function ofrelative position of the first and second members along the line ofadjustment, and having peaks at a plurality of detent positions alongthe line of adjustment; wherein the first member comprises a base, and aprotruding structure on the base having a cylindrical outside surface,wherein the first engagement surface is on the cylindrical outsidesurface; and the second member comprises an opening having a cylindricalinside surface, and wherein the second engagement surface is on thecylindrical inside surface; and wherein the protruding structure has anopening inside the cylindrical outside surface, and further comprisingan electronic component disposed within the opening.
 2. The headset ofclaim 1, wherein the line of adjustment comprises an arc around thecylindrical outside surface.
 3. (canceled)
 4. The headset of claim 1,including a non-magnetic spacer disposed between the first and secondengagement surfaces.
 5. The headset of claim 1, wherein the magneticelements comprise: a plurality of magnets fixed on the first member, andarranged with a magnetic pole proximal to the first engagement surfaceand an opposite magnetic pole distal from the first engagement surface,and wherein the poles of the magnets proximal to the first engagementsurface are disposed in a pattern corresponding to detent positions inthe plurality of detent positions along the line of adjustment; and acomplementary magnetic element on the second member, arranged toincrease the magnetic flux at the plurality of detent positions.
 6. Theheadset of claim 5, wherein one or more of the magnetic elementscomprise an elongated magnetic strip disposed along the cylindricaloutside surface on the first member, and a complementary elongatedmagnetic element on the second member.
 7. The headset of claim 1,wherein one or more of the magnetic elements comprise a patternedmagnetic film fixed on the first member having north and south poles ina pattern proximal to the first engagement surface.
 8. (canceled) 9.(canceled)
 10. The headset of claim 1, wherein the magnetic flux is anattracting force in some relative positions of the first and secondmembers and a repelling force in at least one other relative position.11. A headset, comprising: a headband; a boom hub coupled to theheadband having a first engagement surface; a boom having a secondengagement surface, the second engagement surface disposed for rotationrelative to the first engagement surface of the boom hub; and magneticelements fixed on the boom hub and the boom proximal to the first andsecond engagement surfaces; the magnetic elements arranged to establisha magnetic flux attracting the first engagement surface to the secondengagement surface, the magnetic flux varying as a function of relativeangle of rotation between the first and second engagement surfaces, andhaving peaks at a plurality of detent angles; wherein the boom hubcomprises a base, and a protruding structure on the base having acylindrical outside surface, wherein the first engagement surface is onthe cylindrical outside surface; and the boom comprises an openinghaving a cylindrical inside surface, and wherein the second engagementsurface is on the cylindrical inside surface; and wherein the protrudingstructure has an opening inside the cylindrical outside surface, andfurther comprising an electronic component disposed within the opening.12. The headset of claim 11, including a non-magnetic spacer disposedbetween the first and second engagement surfaces.
 13. The headset ofclaim 11, wherein the magnetic elements comprise: a plurality of magnetsfixed on the boom hub, and arranged with one magnetic pole proximal tothe first engagement surface and an opposite magnetic pole distal fromthe first engagement surface, and wherein the poles of the magnetsproximal to the first engagement surface are disposed in a patterncorresponding to detent angles in the plurality of detent angles; and acomplementary magnetic element on the boom, arranged to increase themagnetic flux at the plurality of detent angles.
 14. The headset ofclaim 11, wherein one or more of the magnetic elements comprise apatterned magnetic film fixed on the boom hub having north and southpoles in a pattern proximal to the first engagement surface. 15.(canceled)
 16. (canceled)
 17. The headset of claim 11, wherein theelectronic component comprises a push button switch.
 18. The headset ofclaim 11, wherein the magnetic flux is an attracting force in somerelative positions of the boom hub and the boom and a repelling force inat least one other relative position.
 19. (canceled)
 20. (canceled) 21.(canceled)
 22. (canceled)
 23. (canceled)